Singlet–Triplet Splittings in the Luminescent Excited States of Colloidal Cu+:CdSe, Cu+:InP, and CuInS2 Nanocrystals: Charge-Transfer Configurations and Self-Trapped Excitons
Abstract:The electronic and magnetic properties of the luminescent excited states of colloidal Cu(+):CdSe, Cu(+):InP, and CuInS2 nanocrystals were investigated using variable-temperature photoluminescence (PL) and magnetic circularly polarized luminescence (MCPL) spectroscopies. The nanocrystal electronic structures were also investigated by absorption and magnetic circular dichroism (MCD) spectroscopies. By every spectroscopic measure, the luminescent excited states of all three materials are essentially indistinguish… Show more
“…46 However, recent work has
unambiguously demonstrated that the PL in CP CIS QDs originates from
the radiative recombination of a delocalized CB electron with a hole
localized on a Cu + ion. 31,47,48 Nevertheless, the nature of the hole localization
process (i.e., self-trapping onto a regular Cu + ion 48 or capture by a native defect, such as Cu In 2– ) has yet to be unravelled. 31 …”
Copper indium sulfide
(CIS) quantum dots (QDs) are attractive as
labels for biomedical imaging, since they have large absorption coefficients
across a broad spectral range, size- and composition-tunable photoluminescence
from the visible to the near-infrared, and low toxicity. However,
the application of NIR-emitting CIS QDs is still hindered by large
size and shape dispersions and low photoluminescence quantum yields
(PLQYs). In this work, we develop an efficient pathway to synthesize
highly luminescent NIR-emitting wurtzite CIS/ZnS QDs, starting from
template Cu2-xS nanocrystals (NCs),
which are converted by topotactic partial Cu+ for In3+ exchange into CIS NCs. These NCs are subsequently used as
cores for the overgrowth of ZnS shells (≤1 nm thick). The CIS/ZnS
core/shell QDs exhibit PL tunability from the first to the second
NIR window (750–1100 nm), with PLQYs ranging from 75% (at 820
nm) to 25% (at 1050 nm), and can be readily transferred to water upon
exchange of the native ligands for mercaptoundecanoic acid. The resulting
water-dispersible CIS/ZnS QDs possess good colloidal stability over
at least 6 months and PLQYs ranging from 39% (at 820 nm) to 6% (at
1050 nm). These PLQYs are superior to those of commonly available
water-soluble NIR-fluorophores (dyes and QDs), making the hydrophilic
CIS/ZnS QDs developed in this work promising candidates for further
application as NIR emitters in bioimaging. The hydrophobic CIS/ZnS
QDs obtained immediately after the ZnS shelling are also attractive
as fluorophores in luminescent solar concentrators.
“…46 However, recent work has
unambiguously demonstrated that the PL in CP CIS QDs originates from
the radiative recombination of a delocalized CB electron with a hole
localized on a Cu + ion. 31,47,48 Nevertheless, the nature of the hole localization
process (i.e., self-trapping onto a regular Cu + ion 48 or capture by a native defect, such as Cu In 2– ) has yet to be unravelled. 31 …”
Copper indium sulfide
(CIS) quantum dots (QDs) are attractive as
labels for biomedical imaging, since they have large absorption coefficients
across a broad spectral range, size- and composition-tunable photoluminescence
from the visible to the near-infrared, and low toxicity. However,
the application of NIR-emitting CIS QDs is still hindered by large
size and shape dispersions and low photoluminescence quantum yields
(PLQYs). In this work, we develop an efficient pathway to synthesize
highly luminescent NIR-emitting wurtzite CIS/ZnS QDs, starting from
template Cu2-xS nanocrystals (NCs),
which are converted by topotactic partial Cu+ for In3+ exchange into CIS NCs. These NCs are subsequently used as
cores for the overgrowth of ZnS shells (≤1 nm thick). The CIS/ZnS
core/shell QDs exhibit PL tunability from the first to the second
NIR window (750–1100 nm), with PLQYs ranging from 75% (at 820
nm) to 25% (at 1050 nm), and can be readily transferred to water upon
exchange of the native ligands for mercaptoundecanoic acid. The resulting
water-dispersible CIS/ZnS QDs possess good colloidal stability over
at least 6 months and PLQYs ranging from 39% (at 820 nm) to 6% (at
1050 nm). These PLQYs are superior to those of commonly available
water-soluble NIR-fluorophores (dyes and QDs), making the hydrophilic
CIS/ZnS QDs developed in this work promising candidates for further
application as NIR emitters in bioimaging. The hydrophobic CIS/ZnS
QDs obtained immediately after the ZnS shelling are also attractive
as fluorophores in luminescent solar concentrators.
“…Upon photoexcitation, the 1S holes nonradiatively moved from the valence band to the impurity in the core 30. The luminescence of the g‐QDs is attributed to the radiative recombination of the conduction band 1S electrons with the impurity holes 30.…”
Colloidal heterostructured quantum dots (QDs) are promising candidates for next‐generation optoelectronic devices. In particular, “giant” core/shell QDs (g‐QDs) can be engineered to exhibit outstanding optical properties and high chemical/photostability for the fabrication of high‐performance optoelectronic devices. Here, the synthesis of heterostructured CuInSexS2−
x (CISeS)/CdSeS/CdS g‐QDs with pyramidal shape by using a facile two‐step method is reported. The CdSeS/CdS shell is demonstrated to have a pure zinc blend phase other than typical wurtzite phase. The as‐obtained heterostructured g‐QDs exhibit near‐infrared photoluminescence (PL) emission (≈830 nm) and very long PL lifetime (in the microsecond range). The pyramidal g‐QDs exhibit a quasi‐type II band structure with spatial separation of electron–hole wave function, suggesting an efficient exciton extraction and transport, which is consistent with theoretical calculations. These heterostructured g‐QDs are used as light harvesters to fabricate a photoelectrochemical cell, exhibiting a saturated photocurrent density as high as ≈5.5 mA cm−2 and good stability under 1 sun illumination (AM 1.5 G, 100 mW cm−2). These results are an important step toward using heterostructured pyramidal g‐QDs for prospective applications in solar technologies.
“…24,25 Furthermore, impurity doping of perovskite thin films has been shown
to improve their performance in solar cells. 26−28 Recently, Mn 2+ doping in colloidal CsPbCl 3 perovskite NCs has
been achieved by a direct synthesis method, in which PbCl 2 and MnCl 2 precursors were mixed in the desired ratio,
leading to NCs with the characteristic Mn 2+ emission.…”
Colloidal
CsPbX3 (X = Br, Cl, and I) perovskite nanocrystals
(NCs) have emerged as promising phosphors and solar cell materials
due to their remarkable optoelectronic properties. These properties
can be tailored by not only controlling the size and shape of the
NCs but also postsynthetic composition tuning through topotactic anion
exchange. In contrast, property control by cation exchange is still
underdeveloped for colloidal CsPbX3 NCs. Here, we present
a method that allows partial cation exchange in colloidal CsPbBr3 NCs, whereby Pb2+ is exchanged for several isovalent
cations, resulting in doped CsPb1–xMxBr3 NCs (M= Sn2+, Cd2+, and Zn2+; 0 < x ≤ 0.1), with preservation of the original NC shape. The size
of the parent NCs is also preserved in the product NCs, apart from
a small (few %) contraction of the unit cells upon incorporation of
the guest cations. The partial Pb2+ for M2+ exchange
leads to a blue-shift of the optical spectra, while maintaining the
high photoluminescence quantum yields (>50%), sharp absorption
features,
and narrow emission of the parent CsPbBr3 NCs. The blue-shift
in the optical spectra is attributed to the lattice contraction that
accompanies the Pb2+ for M2+ cation exchange
and is observed to scale linearly with the lattice contraction. This
work opens up new possibilities to engineer the properties of halide
perovskite NCs, which to date are demonstrated to be the only known
system where cation and anion exchange reactions can be sequentially
combined while preserving the original NC shape, resulting in compositionally
diverse perovskite NCs.
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